Katherine Freese’s research while affiliated with University of Texas at Austin and other places

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Publications (367)


FIG. 3. Updated range of portal couplings κ allowed by the freeze-in scenario (labeled "Freeze-in Region") when accounting for reheating temperatures T rh ≲ m χ . The previously understood freeze-in benchmark with T rh ≫ m χ corresponds to the bottom solid green line. Shaded in gray are the current experimental constraints from PandaX [2] and XENON1T [3,4].
Minimal dark matter freeze-in with low reheating temperatures and implications for direct detection
  • Article
  • Full-text available

March 2025

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3 Citations

Physical Review D

Kimberly K. Boddy

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Katherine Freese

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Barmak Shams Es Haghi

We investigate the influence of the reheating temperature of the visible sector on the freeze-in dark matter (DM) benchmark model for direct detection experiments, where DM production is mediated by an ultralight dark photon. Here, we consider a new regime for this benchmark: we take the initial temperature of the thermal Standard Model (SM) bath to be below the DM mass. The production rate from the SM bath is drastically reduced due to Boltzmann suppression, necessitating a significant increase in the portal coupling between DM and the SM to match the observed relic DM abundance. This enhancement in coupling strength increases the predicted DM-electron scattering cross section, making freeze-in DM more accessible to current direct detection experiments. Published by the American Physical Society 2025

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The Simons Observatory: Science Goals and Forecasts for the Enhanced Large Aperture Telescope

March 2025

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6 Reads

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I. Abril-Cabezas

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[...]

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I. Zubeldia

We describe updated scientific goals for the wide-field, millimeter-wave survey that will be produced by the Simons Observatory (SO). Significant upgrades to the 6-meter SO Large Aperture Telescope (LAT) are expected to be complete by 2028, and will include a doubled mapping speed with 30,000 new detectors and an automated data reduction pipeline. In addition, a new photovoltaic array will supply most of the observatory's power. The LAT survey will cover about 60% of the sky at a regular observing cadence, with five times the angular resolution and ten times the map depth of Planck. The science goals are to: (1) determine the physical conditions in the early universe and constrain the existence of new light particles; (2) measure the integrated distribution of mass, electron pressure, and electron momentum in the late-time universe, and, in combination with optical surveys, determine the neutrino mass and the effects of dark energy via tomographic measurements of the growth of structure at z<3z < 3; (3) measure the distribution of electron density and pressure around galaxy groups and clusters, and calibrate the effects of energy input from galaxy formation on the surrounding environment; (4) produce a sample of more than 30,000 galaxy clusters, and more than 100,000 extragalactic millimeter sources, including regularly sampled AGN light-curves, to study these sources and their emission physics; (5) measure the polarized emission from magnetically aligned dust grains in our Galaxy, to study the properties of dust and the role of magnetic fields in star formation; (6) constrain asteroid regoliths, search for Trans-Neptunian Objects, and either detect or eliminate large portions of the phase space in the search for Planet 9; and (7) provide a powerful new window into the transient universe on time scales of minutes to years, concurrent with observations from Rubin of overlapping sky.


Higgs Inflation and the Electroweak Gauge Sector

March 2025

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6 Reads

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2 Citations

Fortschritte der Physik

We introduce a method that allows the Higgs to be the inflaton. The Higgs is considered as a pseudo‐Nambu‐Goldstone (pNG) boson of a global coset symmetry , which is spontaneously breaks at an energy scale . A suitable Chern−Simons (CS) interaction is given to it, with representing the dimensionless CS coupling strength and an decay constant. As a result, slow‐roll inflation occurs via ‐induced friction down a steep sinusoidal potential. To obey electroweak symmetry, the lowest‐order CS interaction is required to be quadratic in the Higgs, with the coupling strength . Higher‐order interaction terms keep the full Lagrangian nearly invariant under the approximate pNG shift symmetry. Employing the simplest symmetry coset , ‐folds of inflation occur when . Successfully explaining inflation necessitates small values of the decay constant, ; this in turn requires large , which is ruled out by electric dipole measurements. Although the electroweak hierarchy problem while achieving successful inflation, the real benefit is found in providing a different path to identifying the Higgs as the inflaton, outside the standard modified‐gravity framework.


Free-Streaming Neutrinos and Their Phase Shift in Current and Future CMB Power Spectra

January 2025

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5 Reads

The cosmic neutrino background and other light relics leave distinct imprints in the cosmic microwave background anisotropies through their gravitational influence. Since neutrinos decoupled from the primordial plasma about one second after the big bang, they have been free-streaming through the universe. This induced a characteristic phase shift in the acoustic peaks as a unique signature. In this work, we constrain the free-streaming nature of these relativistic species and other light relics beyond the Standard Model of particle physics by establishing two complementary template-based approaches to robustly infer the size of this phase shift from the temperature and polarization power spectra. One template shifts the multipoles in these spectra, while the other novel template more fundamentally isolates the phase shift at the level of the underlying photon-baryon perturbations. Applying these methods to Planck data, we detect the neutrino-induced phase shift at about 10σ10\sigma significance, which rises to roughly 14σ14\sigma with additional data from the Atacama Cosmology Telescope and the South Pole Telescope. We also infer that the data is consistent with the Standard Model prediction of three free-streaming neutrinos. In addition, we forecast the capabilities of future experiments which will enable significantly more precise phase-shift measurements, with the Simons Observatory and CMB-S4 reducing the 1σ1\sigma uncertainties to roughly 4.3% and 2.5%, respectively. More generally, we establish a new analysis pipeline for the phase shift induced by neutrinos and other free-streaming dark radiation which additionally offers new avenues for exploring physics beyond the Standard Model in a signature-driven and model-agnostic way.



Dark Matter Production during Warm Inflation via Freeze-In

November 2024

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19 Reads

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3 Citations

Physical Review Letters

We present a novel perspective on the role of inflation in the production of dark matter (DM). Specifically, we explore the DM production during warm inflation via ultraviolet freeze-in (WIFI). We demonstrate that in a warm inflation (WI) setting the persistent thermal bath, sustained by the dissipative interactions with the inflaton field, can source a sizable DM abundance via the nonrenormalizable interactions that connect the DM with the bath. Compared to the (conventional) radiation-dominated (RD) UV freeze-in scenario for the same reheat temperature (after inflation), the resulting DM yield in WIFI is always enhanced showing a strongly positive dependence on the mass dimension of the nonrenormalizable operator. Of particular interest, for a sufficiently large mass dimension of the operator, the entirety of the DM abundance of the Universe can be created during the inflationary phase. For the specific models we study, we find that the enhancement in DM yield, relative to RD UV freeze-in, is at least an order of magnitude for an operator of mass dimension 5, and as large as 18 orders of magnitude for an operator of mass dimension 10. Our findings also suggest a broader applicability for producing other cosmological relics, which may have a substantial impact on the evolution of the early Universe. Published by the American Physical Society 2024


FIG. 1. In slow-roll inflation (left panel) the inflaton rolls down its potential. In chain inflation it tunnels from minimum to minimum in its potential.
FIG. 3. Evolution of the vacuum and radiation energy densities in chain inflation scenarios with and without a postinflationary phase transition. In the left panel one slower phase transition occurs after inflation [boundary condition (i)], corresponding to scenario 1 of Fig. 2. The Universe becomes vacuum-dominated for a second (short) period before the last transition transfers the remaining vacuum energy into radiation. In the right panel inflation ends by the last phase transition and the Universe immediately enters the standard radiation-dominated epoch [boundary condition (ii)], corresponding to scenario 2 of Fig. 2. In the above figures the duration of the phase transitions has been neglected. The following parameters were chosen: V 1=4 Ã ¼ 10 8 GeV, ΔV 1=4 ¼ 2.7 × 10 6 GeV, Γ 1=4 Ã =H Ã ¼ 3.0 × 10 4 , S 1 ¼ −2, S 2 ¼ 4, S 3 ¼ 3, S 4 ¼ 1 and α ¼ 10 (α ¼ 0) in the left (right) panel.
FIG. 5. Amplitude and power law index consistent with the gravitational wave signal observed at several PTA experiments (2σ-contours). The published NANOGrav signal regions for the 15-and 12.5-yr datasets are shown in dark and light blue. The pink contour was derived with our Δχ 2 -test to the NANOGrav 15-yr data. The blue and yellow regions were obtained by the PPTA and EPTA experiments. Hence this figure shows that our statistical method upon the data accurately reproduces results previously published by the NANOGrav collaboration.
Gravitational wave spectrum of chain inflation

November 2024

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15 Reads

Physical Review D

Chain inflation is an alternative to slow-roll inflation in which the inflaton tunnels along a large number of consecutive minima in its potential. In this work we perform the first comprehensive calculation of the gravitational wave (GW) spectrum of chain inflation. In contrast to slow-roll inflation the latter does not stem from quantum fluctuations of the gravitational field during inflation, but rather from the bubble collisions during the first-order phase transitions associated with vacuum tunneling. Our calculation is performed within an effective theory of chain inflation which builds on an expansion of the tunneling rate capturing most of the available model space. The effective theory can be seen as chain inflation’s analog of the slow-roll expansion in rolling models of inflation. The near scale-invariance of the scalar power spectrum translates to a quasiperiodic shape of the inflaton potential in chain inflation, with the tunneling rate changing very slowly during the e-folds leading to cosmic microwave background observables. We show that chain inflation produces a very characteristic double-peak GW spectrum: a faint high-frequency peak associated with the gravitational radiation emitted during inflation, and a strong low-frequency peak associated with the graceful exit from chain inflation (marking the transition to the radiation-dominated epoch). There exist very exciting prospects to test the gravitational wave signal from chain inflation at the aLIGO-aVIRGO-KAGRA network, at LISA and /or at pulsar timing array experiments. A particularly intriguing possibility we point out is that chain inflation could be the source of the stochastic gravitational wave background recently detected by NANOGrav, PPTA, EPTA, and CPTA. We also show that the gravitational wave signal of chain inflation is often accompanied by running/ higher running of the scalar spectral index to be tested at future cosmic microwave background experiments. Published by the American Physical Society 2024


Figure 1. Globally-averaged H ionized fraction, ⟨x HII ⟩, vs. redshift z, from the Cosmic Dawn II simulation. Black points show the hydrogen ionization fraction of snapshots at different redshifts from the CoDa II simulation, averaged over the simulation volume. The curve connecting them represents a cubic spline fit to these points. In this model, reionization is largely completed around redshift z ≈ 6, and the universe is half-ionized around redshift z ≈ 7.
Figure 2. Diagram comparing the time between Cosmic Dawn (CoDa) II simulation snapshots and those in the CoDa II-Dark Matter simulation. From the CoDa II simulation, we averaged over multiple simulated snapshots in the time it takes light to cross any one simulation volume, while from the CoDa II-Dark Matter simulation, we interpolated between two consecutive simulation snapshots to construct a synthetic snapshot. Therefore, we approach the process of creating synthetic snapshots based off of these two simulations in slightly different manners, described in detail in the main text and shown diagrammatically in the sequences labelled 'CoDa II' and 'CoDa II-Dark Matter'. Ultimately, our goal in both cases is to generate a series of synthetic snapshots based off the simulation results but spaced in time in such a way that the time between snapshots is exactly the time it takes light to travel across the simulation volume, as depicted in the sequence labelled 'Target'.
Figure 3. Mean of dispersion measures modeled from CoDa II/CoDa II-Dark Matter simulations. The solid blue curve shows the mean of the dispersion measures constructed from the CoDa II/CoDa II-Dark Matter simulations of FRBs whose source is located at a range of redshifts 0 < z < 12. The orange dashed curve is the mean under the assumption that the universe is fully ionized over that entire redshift range, specifically using the CoDa II density fields at redshifts z > 5.8 and CoDa II-Dark Matter at lower redshifts. The red dash-dotted curve shows the mean if we spatially average the ionization field from the CoDa II simulation, while retaining the CoDa II density field, allowing us to estimate the effects of the globally-averaged rise of the ionized fraction as the universe reionized, treated as a non-patchy (i.e. uniform), evolving, partial ionization. The means in these three cases are indistinguishable from z = 0 out to the epoch of reionization, at which point a plateau appears in the CoDa II patchy and nonpatchy reionization cases, where the globally-averaged hydrogen ionized fraction drops below unity at z ≳ 6 (as shown in Fig. 1). We also plot the results from Jaroszynski (2019) as a comparison (black points) found using the data from the Illustris simulation. A slight difference between the results in Jaroszynski (2019) and the two results we construct for the mean arises because we include a period of helium reionization at redshift z = 3.
Figure 6. Average hydrogen ionization histories (⟨x HII ⟩(z)) in each of the reionization histories we consider. As in figure 1, each curve represents the spatially averaged ionization fraction as a function of redshift. The red dash-dotted curve shows the hydrogen ionization history of the CoDa II simulation without modification, which shows the effects of a homogeneous non-patchy reionization. The magenta densely dotted (teal sparsely dotted) curve shows the ionization history if the universe ionized earlier (later) than in the CoDa II simulation, so that the end of reionization is approximately z = 7.1 (z = 5.6). The indigo dash-dot-dotted curve shows the ionization history if reionization occurs in two phases, where 50 per cent of the universe is ionized in each phase, but ionization fraction plateaus between the two phases.
Dispersion Measures of Fast Radio Bursts through the Epoch of Reionization

November 2024

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11 Reads

Dispersion measures (DM) of fast radio bursts (FRBs) probe the density of electrons in the intergalactic medium (IGM) along their lines-of-sight, including the average density versus distance to the source and its variations in direction. While previous study focused on low-redshift, FRBs are potentially detectable out to high redshift, where their DMs can, in principle, probe the epoch of reionization (EOR) and its patchiness. We present the first predictions from large-scale, radiation-hydrodynamical simulation of fully-coupled galaxy formation and reionization, using Cosmic Dawn (``CoDa")~II to model the density and ionization fields of the universe down to redshifts through the end of the EOR at zre6.1z_{re}\approx6.1. Combining this with an N-body simulation CoDa~II--Dark Matter of the fully-ionized epoch from the EOR to the present, we calculate the mean and standard deviation of FRB DMs as functions of their source redshift. The mean and standard deviation of DM increase with redshift, reaching a plateau by z(xHII0.25)8z(x_{HII}\lesssim0.25)\gtrsim8, i.e. well above zrez_{re}. The mean-DM asymptote DMmax5900 pccm3\mathcal{DM}_{max} \approx 5900~\mathrm{pc\, cm^{-3}} reflects the end of the EOR and its duration. The standard deviation there is σDM,max497 pccm3\sigma_{DM, max}\approx497 ~\mathrm{pc\, cm^{-3}}, reflecting inhomogeneities of both patchy reionization and density. Inhomogeneities in ionization during the EOR contribute O(1\mathcal{O}(1 per cent) of this value of σDM,max\sigma_{DM,max} from FRBs at redshifts z8z\gtrsim 8. Current estimates of FRB rates suggest this may be detectable within a few years of observation.


In-Flight Performance of Spider's 280 GHz Receivers

August 2024

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24 Reads

SPIDER is a balloon-borne instrument designed to map the cosmic microwave background at degree-angular scales in the presence of Galactic foregrounds. SPIDER has mapped a large sky area in the Southern Hemisphere using more than 2000 transition-edge sensors (TESs) during two NASA Long Duration Balloon flights above the Antarctic continent. During its first flight in January 2015, SPIDER observed in the 95 GHz and 150 GHz frequency bands, setting constraints on the B-mode signature of primordial gravitational waves. Its second flight in the 2022-23 season added new receivers at 280 GHz, each using an array of TESs coupled to the sky through feedhorns formed from stacks of silicon wafers. These receivers are optimized to produce deep maps of polarized Galactic dust emission over a large sky area, providing a unique data set with lasting value to the field. In this work, we describe the instrument's performance during SPIDER's second flight.



Citations (51)


... Recently, FIMP DM has been studied for the case with a low reheating temperature in Refs. [8][9][10][11][12][13][14][15]. In this case, compared to the standard FIMP DM, DM is much heavier than the reheating temperature, so the thermal production of the DM from the decays and scatterings of thermal particles would be Boltzmann-suppressed. ...

Reference:

Higgs-portal vector dark matter at a low reheating temperature
Minimal dark matter freeze-in with low reheating temperatures and implications for direct detection

Physical Review D

... Recently, the authors in [28] have developed a novel interplay between DM production and inflationary cosmology. They showed that, if a DM-bath coupling of the UV freeze-in type is active during a warm inflationary period, a large abundance of DM is generally produced, with the resulting DM yield typically larger than the standard radiation-dominated UV freeze-in, for the same reheating temperature. ...

Dark Matter Production during Warm Inflation via Freeze-In

Physical Review Letters

... n the early Universe. However, these alternative models struggle to reconcile the observed high SFE approaching 100% at z10 in JWST observations. Dark stars, which inhabit the first dark matter (DM) halos or minihalos in the high-redshift Universe, are fueled by heating from DM (K. Freese et al. 2008Freese et al. , 2016F. Iocco & L. Visinelli 2024;S. Zhang et al. 2024). This heating may originate from the gravitational attraction of DM and the annihilation of DM particles, such as weakly interacting massive particles (WIMPs), which can be captured through elastic scattering with baryonic matter (K. Freese et al. 2010). In the early Universe, DM densities were enhanced by a factor of (1 + z) 3 at reds ...

Detectability of Supermassive Dark Stars with the Roman Space Telescope

The Astrophysical Journal

... To conclude this section we comment on related work. First of all, eternal inflation can be excluded by a future measurement of positive curvature [39] that would exclude an epoch of eternal inflation followed by slow roll, or by a negative running of the spectral index [41,42]. Planck is not sensitive enough to make a definitive statement [43]. ...

Defying eternal inflation in warm inflation with a negative running

... Inflation is typically modeled using a canonical scalar field with a Lagrangian density of the form L = X −V , where X = 1 2 g µν ∂ µ ϕ∂ ν ϕ, and V denotes the inflaton potential. To explore more diverse inflationary scenarios, studies have proposed various models, including those involving noncanonical fields, pure kinetic fields, multi-field models [17][18][19][20][21][22][23][24][25][26], and nonminimal coupling fields [27][28][29], In the past three decades, warm inflation has also undergone significant developments, particularly in microphysical research [30,31], cosmological perturbations [10,30,[32][33][34][35] and model extensions [32,[36][37][38][39]. While most warm inflation models involve canonical fields, exceptions such as the warm Dirac-Born-Infeld (DBI) inflationary model [40], exist. ...

WarmSPy: a numerical study of cosmological perturbations in warm inflation

... Such a level of uncertainty, mainly due to the magnetic field, is extremely low for an astrophysical ALP search and is possible thanks to our detailed knowledge of the solar atmosphere. Other astrophysical limits in the same region of parameter space [58][59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74][75][76] typically come with larger uncertainties, due to the difficulty of modeling ALP production and conversion in far-away astrophysical environments. ...

Constraining axion-like particles with HAWC observations of TeV blazars

... As discussed in the Introduction, astrophysical explanations for these candidates have been put forward. A variety of cosmological explanations beyond ΛCDM have also been considered [45][46][47][48][49][50][51][52][53]. One class of proposals involve a modification of the primordial power spectrum; see, e.g. ...

Supermassive Dark Star candidates seen by JWST
  • Citing Article
  • July 2023

Proceedings of the National Academy of Sciences

... The observed ratio of matter to dark matter, Ω DM ≈ 5 · Ω B , implies a scenario where the baryon charge concealed in antinuggets exceeds that in nuggets by a factor of approximately (ΩN/Ω N ) ≈ 3/2 at the end of nugget formation [19]. Recently, Sebastian Baum et al. proposed a systematic direction for the investigation of neutrino interactions and searches for exotic particles predicted in the extensions of the Standard Model or only phenomenological modelsusing effects in different minerals and rocks [20]. ...

Mineral detection of neutrinos and dark matter. A whitepaper

Physics of the Dark Universe

... Current constraints on isocurvature [2] typically assume its power spectrum follows a simple power law as a function of perturbation wavenumber, as is naturally expected in axion or curvaton models (for reviews, see e.g., [3,4]). However, numerous well-motivated new physics scenarios -such as cosmological phase transitions [5][6][7] and gravitational particle production during inflation [8][9][10][11][12][13][14][15] -predict isocurvature power spectra that deviate from this assumption. Limits derived under the assumption of a power law cannot straightforwardly be applied to models with different power spectra. ...

Dark matter and gravitational waves from a dark big bang

Physical Review D